Electric measuring and protecting device



.July 28, 1931. A. D. n lovlcl AELlEC'lRIC MEASURING AND PROTECTING DEVICE Filed Dec. 21. 1927 4 sheets-sheet '1 A ry 12J LLM Az n July 28, 1931. A. D. n lovlcl 1',816778 ELECTRIC MEASURING AND PROTECTING DEVICE Filed neo. 21, 1927 4'sheetS-sneet 2 July 28, 1931. A. D. n lovlcl 1,816,778

ELECTRIC MEASURING AND PROTECTING DEVICE Filed Dec. 21, 1927 4 Sheets-Sheet 4 Patented July 28, 1931 UNITED srrresr PATENT Aorrlcl:

AVRAM DAVID ILIOVICI, 0F PARIS,KFRANCE, ASSIGNOR, BY ASSIGNMENTS, T0 GENERAL ELECTRIC COMPANY, A CORPORATION OF NEW YORK ELECTRIC MEASURING AND PROTECTING DEVICE Application filed December 21, 1927, Serial No. 241,622, and in France January 7, 1927.

The present invention relates to electric circuit protecting or measuring instruments which are subjected to torques which are functions of any one or more of the phase seqluence components of the power or other e ectric quantity involved.

One object of the present invention is to provide circuit arrangements and apparatus for producing two torques which are funcltions of any one or more of the phase sequence components of the power in the circuit which is to be protected or which is under measurement, whereby the sum of or the difference between said torques is made to act on a movable element in such a manner that the relative value or values of one or more of thel phase sequence components in the function representing the resultant torque shall be diminished. c y

A further obj ect of the present invention is to adjust the aforementioned torques in such wise that either one or two of the phase sequence components of the power shall vanish completely from the function representing their resultant.

There are a number of 'ways of designing apliaretus for polyphase circuits wherein the torque acting on the movable element depends on the useful power or the wattless power, or, speaking generally, on an intermediate component which we shall call the complex power, Pa of the circuit.

By complex power vof angle ay is understood the quantity Pa having the form in the case of a two-wire single phase circuit, the currents and voltages being of sinusoidal wave-form,(I and E arethe root-mean-square or effective values of the current and voltage, the phase angle between these quantities an d a an angle which represents the angular departure in a given direction from the in-phase relationship of current and voltage at which the apparatus has maximum torque and which may he positive or negative, for example, in a w'attmeter 1:00 and in a reactive kva. meter a: i900). In polyphase circuits, the expression Pa is deduced from the formula (l) in the Vsame way as the useful power or the wattless power is deduced from the formulae P=EI COS (1) PW=EI sin qS (1),

is true, denoting any complex power (in particular a useful power or a wattless power) by Pa and the positive, negative and zero phase sequence components of this power by Pad, Pai and Pao; and A, a coefficient. A23 for three-phase systems and A=2 for two-phase systems. Often PaOZO that is when there is no leakage current or the apparatus does notrespond to the Zero phase sequence compoand nent of the power, for example, in the two wattmetcr connection for measuring power.

If therefore the torque of the apparatus is a function of the power, irrespective of the degree of .imbalance of the currents or voltages: Y

where 7c is practically a constant. For the sake of simplicity this case only will be considered, but it'should be understood that the invention applies to the most general casc.

If the instantaneous values of the voltages to ground of the conductors of a three-phase circuit are el, c2, e3 and the currents in the corresponding c onductors il, 2, i3 then, as is known, these may be expressed in terms of their positive, ynegative and Zero phase se- 4ret constitutes what is called a fluctuating energy which is a double frequency Ijinlsation. tects in accordance with Equation (4") are All the methods which measure correctly the power of a three-phase circuit, theret'orel measure the sum ot the positive, negative and zero phase sequence power components, tor example P or a torque dependent thereon can be obtained by making a correct measurement of the total power of the circuit with the three wattmeter connection and the positive and negative components with the two wattmeter connection.

It the relation between torque and power, that is CSWPQ, n being a constant, holds good only when at least one ot' the systems, voltage or current, is balanced, this torque will always be a function of certain complex powers Pad, Pai, Poe/H which may correspond to diHerent values ot angle a, Pad being a positive phase sequence component of power, Pai being a negative phase sequence component o1"l power and Pao" a Zero phase sequence component of the power. Thus, if there is taken the sum of the vectorial products of each current by the opposite line to line voltage, that is the voltage in quadrature to the current under balanced circuit conditions, there results:

Eid-2]?, sin (l5/a, (ibi, '/zg (,b/z. being the angles between respecti rely associated voltages and currents. This can be expressed (ZL-i2 El) I3 Sin bis or using the phase sequence components ol" the currents and voltages as But according to the phase sequence component theory:

-mla

jy gEt-,-

Egd-"Eld Substituting in (9), there results:

Methods and apparatus 'for obtaining efthe resultant torque.

described in connection with the several figures of the" drawings.

In particular, in the case corresponding to formula (3') a, b and c being constants U: aPad bPa. cPao" (4) If rthe sum of or the difference between two torques, one of' form or (3') and the other of form (4) (or of the general form corresponding thereto in the case of non proportionality) or both of form (4), be applied to the movable element, the component torques can, by a suitable choice of design characteristics, be adjusted in order to cause one of the symmetrical components to vanish from Thus, if there be provided, as in accordance with my invention, apparatus responsive to a resultant of two effects, such as the sum of or the difference between the functions set forth in Equations (3) and (4), operation dependent on at least one phase sequence component follows since from the sum, Pi-P, there results:

Pl P P=P 1 2 .1+ Jrw/B and if P0=0 Pl P (P d t +Je, and from the difference, P-P

Pl 2P1-l-Po and if PO=0 P P- -.(P-V

Generally the ositive phase sequence component will be eliminated and the torque will then depend on only the negative and zero phase sequence components. As it is easy to cause this latter to vanish, it will then be possible to influence the apparatus solely by the negative phase sequence component of' the power. It is likewise possible to obtain a torque depending solely on the positive or zero phase sequence component. Moreover, matters may be arranged so that the component or components which have not been eliminated shall correspond to any desired complex power as will hereinafter appear.

The present invention relates to measuring or protecting apparatus, wattmeters, other meters, relays and the like, in which the prineiples set forth above are applied. The desired results will be obtained by a suitable choice of the currents and voltages acting on the windings of the apparatus, by producing suitable phase angle displacements between the currents in said windings, or between the magnetic fluxes they produce and the voltages or the currents in the phases of the circuit which is to be protected 0r which is under measurement.

The various phase angle displacements will be obtained by using reactance coils, capacities, short-circuited rings or circuits, trans,- formers or any other suitable means.

MyV invention will be better understood from the following description when considered in connection with the accompanying drawings and its scope will be pointed out in the appended claims.

In the drawings:

Fig. 1 illustrates diagrammatically a wattinetcr connected in a four-wire three-phase system for producinga torque of the forni e (Pd-enero).

Fig. 2 illustrates diagrainiiiatieally how a wattmetric device similar to that of Fig. 1 is connected to produce a torque of the form lc (Pd-Pi).

Fig. 3 illustrates a circuit arrangement similar to that of Fig. 1 except that the voltage coils are connected to an artilicial or ungronnded neutral point.

Figs. 4 and 5 illustrate circuit arrangements Vsimilar to those of Figs. 3 and 2 for a three-wire three-phase circuit.

Figs. 6 and 7 show diagramiiiatically how the circuit arrangements of Figs. 4 and 5 can be applied to the circuit measuring or protecting apparatus. Y

Figs. 8 and 9 show diagrammatically circuit arrangements for the electro-magnets acting on the rotating element.

Figs. 10 and 11 show two other circuit arrangements.

Fig. 12 illustrates diagrammatically an embodiment of my invention according to the arrangements shown in Figs. 1 and 2;

Figs. 13 and 14 illustrate diagramniatically modifications, in accordance with Figs. 8 and 9 respectively, of theembodiment of my iiiveiition shown in Fig. 6.

Fig. 15 illustrates diagrainniatically a modification of the embodiment of my invention shown in Fig. 12, connected in accordance with Figs. 10. and' 11.

Fig. 16 illustrates diagrammatically another modification of my invention.

In the first case, a 4-'wire three-phase circuit will be considered, and it will be assumed that an induction device which is similar to a wattnieter and which comprises three electro-magnets or motoring devices including the elements El, E2, as shown in Fig. 12 for a 4-wire circuit is used. The'appa'ratus being connected according to the wiring dia` gram of F ig. 1, the movable element including the disks d is subjected to a torque of the form In Fig. l, 1, 2 and 3 are the three line wires and 4 the neutral wire; N is the neutral point; A1, A2, A3, the current coils of the three electro-magnets of the apparatus; V1, V2, V3, their voltage coils. The torque effect ofeach of the motoring elements E1 E2 will be substantially proportional to the product ofV the voltage and the current,v

energizing the respectively associated windings and the cosine of the phase angle between such voltage and current.

Three other electro-magnets or motoring devices, including the elements El, Eg, as shown in Fig. l2, of wattless power or reactive kva. measuring wattmetric devices (e. g. electro-magnets, the current coils of which are connected iri similar manner to those ot the preceding electro-magnets El, El, but the voltage coils oi" which have a negligible reactance in comparison with their resistance) are caused to act on the same movable element including the disks Z or on an element mei^hanically coupled to it. The coils of these electro-magnets El, Eg are connected according to the wiring diagram of Fig. 2, in which l, 2 and 3 are the line wires; l the neutral wire and N the neutral point; Al, iig., AC; are the current coils of the electroniagnets; Vl, Vg, Vg their voltage coils. rlhe torque ol each ot the motoring devices E. E@ will be substantially proportional to the product of the voltage and the current, energizing the respectively associated windin and the sine of the phase angle between such voltage and current. In order that the voltage coils may have a negligible reactance in comparison with their resistance or, in other words, that the current in the voltage coils may be in phase with the voltage, suitable phase displacingr means such as resistors fr may be used.

ln the first circuit arrangement (Fig. 1,) the torque exerted by the motoring elements Fil E2 (Fig. l2) and acting on the movable equipment Z is of the form:

lWhere Pd is the positive phase sequence component ot the useful power and Fi and P the negative and zero phase sequence componeifits thereof respectively.

lilith the last-mentioned circuit arrangement (namely that o'l Fig. 2,) the torque exerted b v the motoring elements El E@ (Fig. l2) is:

@flared-P.) (e) assuming that matters are so arranged that same constant obtains for C1 and C2. e two torques are made to act on the same movable element, :tor example the shaft supporting the disks (l in Fig. l2, in opposition to each other, the resultant torque will be:

ebt-ain an operation dependent upon the sum of the negative and the zero phase sequence components of the power. It' the electroresponsive device according to Fig. 12 is for protective purposes, the contacts c may be arranged to control the circuitof a trip coil t of a circuit breaker since abnormal circuit conditions such as phase unbalance, short-circuits and grounds usually result in negative phase sequence power and, lin case ot grounds, also zero phase sequence power. invention is, of course, not limited to such arrangements but obviously includes the use ot' the rotation of the disks I or their common shaft to drive a recording mechanism such as is used in watt-hour meters.

It the circuit arrangement of Fig. f-l in which the three voltage circuits, assumed to be identical, are connected to an artificial or isolated neutral point 0 be substituted for that of Fig. l, that is the common point olE the voltage windings V1. V2, V3 of Fig. l2 is not grounded, then the F0 term of Equation disappears and UFMPHP.) (5') and the torque C assuming C1 ol Equation (5') and Cu ol' Equation (6) to act in opposition on the same movable element, becomes The apparatus is subjected to only the negative phase sequence componentof the power.

The circuit arrangements may be simplified if the relations holding between the voltages be taken into account (e. g. that the sum ol the line voltages is zero or that the sum of the phase yvoltages is zer-o as in the case ot Fig. 2l) or the relations holding between the currents (the sum et the currents is Zero in three wire ungrounded circuits). Thus, tor three wire circuits, the circuit arrangements otl Figs. 3 and 2 may he replaced h v the two coil. arrangements o'l Figs. s; and respectively in which the reference letters have the saine meaning as in Fig.. 3 and 2,' O being an artilicial or isolated neutral point and r, 1', fr three noninductive resistances.

Fig. 6 is a diagrammatic view of an apparatus which can be connected as indicated in Figs. 4 and 5. The apparatus is connected in the circuit as shown in Figs. 6 and T. ln these figures, A1 BL and A2 B2 representl the two highly inductive voltage circuits A. B1 and Ag B.. the two noninductive voltage circuits;

C1 DMF/2 D2, C 1 Dl. Cg D@ the current circuits; Z and d two metallic disks.

nz E2 represent the y neutral wire, N the neutral point,v O the point common to the three circuits V1, V2, V3.

In Fig. 11, A1,A2, As are the current circuits and Vl, V2, V3 the voltage circuits of the electro-magnets.

The arrangements shown in Figs. 10 and 11 may be carried out constructionally as shown diagrammatically in Fig. 15 after the manner described for Figs. 1 and 2 as shown in Fig. 12. In Fig. 1, the current I1 is associated with the voltage Ei, but in Fig. 10, it

` spect to rthose of the voltage circuits of the electro-magnets by (l1-1209) in the circuit arrangement of Fig.y 10, and by (a+1200) in the circuit arrangement of Fig. 11, that is the fluxes derived from E1 are out of phase with the fluxes derivedl from I1 by (a- 1200) and (ai-1200) in Figs. 10 and 11` respectively and similarly for the fluxes Aderived from E2, I2 and E3, I3, and if furthermore the two electro-magnet systems E1 E2,E1 'i E2 are made to action the same movable element m, as shown in Fig. 15, and if their torques arevadjusted so as to obtain a zero resultant torque when the voltages or currents are balancedy then, when the voltages and currents are unbalanced there will be a Y where Pa, and Pa., are respectively the negative and zero phase sequence components of the power.

If instead of connecting the point .O of Fig. 10 .to the point N, an artificial or isolated neutral point is made, Pao vanishes and t-he torque of the apparatus assumes the form Ozlpai.

' The three wattmetric elements may be replaced by two if' the relationsy between the currents are taken into account as will be obvious from the description in connection with Figs. t to 9 inclusive.

Instead however of eliminating one or two of the phase sequence components of the power, it may be of interest only to reduce the value of one of such phase sequence components with respect to the others. Thus, if for example the movable element is subjected to atorque of forni 0127(Pgi-Pihpg) and; to another' of form 02:70/(PfzNPi) where Pd, Pi and P., have the same meaning as heretofore, and le, la are two positive constants depending for example on the design characteristics of the apparatus, a resultant torque may be obtained of the form:

and, if the voltages or currents have a zero resultant that is to say, zero phase power does not affect the device as in Figs. 3 and 4 for. example then:

0: (7a-11') 121+ (a+/MP.-

lVhen :71:', the expression narrows down to Formula (7') given above and the component Pd vanishes. But if kik', the value of the component Pd is merely diminished with respect to that of the component Pi. In this way, for example, the devices may be highly sensitive to negative phase sequence power which accompaniesphase unbalance and yet sufliciently sensitive to positive phase sequence power to insure operation on large balanced currents, such as may occur in case of a three-phase short-circuit. Also, if (U-e) is relatively small, then the effect of balanced loads on the device is diminished so that under abnormal conditions the devices become more discriminating than the known types of power responsive devices.

This method of reducing the value of one component with respect to the others may be made use of in connection with all the eX- amples discussed above, as it is merely a question of design constants. I

The utilization of the phase and line voltages obtaining in the circuit and of the phase or line currents has been considered in the proceeding. It is also )ossible to use voltages of the form U= aUwLbU) where `U and U are vectors designating two of the circuit voltages, Ya and being positive' or negative constants. Voltages of the form U may be obtained byy means of transformers or auto-transformers, fed by the voltages of the system, or by means of transformersor auto-trans'formers of the rotating field type. Thus, for example as shown in Fig. 16 which is a modification of my invention similar to F ig." 6, a voltage E2,1 directly proportional `to the voltage on thev i u Lu.

coil AlBl ot Fig. 6 can be obtained where suitable means such as a standelta potential trans former 2l forms a part or the available equipment by connecting the coil All so that it is energized in accordance with the sum of the voltages El and l-E, since this sum is ll-E11. Similarly the coil A. .B2 is connected to be energized in accordance with the sum oitl the if'oltages ICQ and El this sum being fl-Em.

Similarly currents or ampere-turns may be used oit the form ((rfIiZ/I) where I and I are vectors of two oi the line or phase currents, o and i5 being` positive or negative constants.

Ampere-turns or currents of the above form may be obtained in several ways. For instance a double winding may be used, one of the windings having' the current I ilowing through it, the other the current I, the two windings having` the same or an unequal number of turns which may be wound in the same or in opposite directions. F or example, as shown in F ig. i6 it may be necessary to obtain the currents, Il and I3 ol the circuit l, 2, 3, desired in the current coils ot the upper and lower elements oit the device from a line l', 2', 8 fed through a stardelta power transformer This can be done by current transformers Q3, 24 and 25 so connected to energize the two-part current coils 26, 27 and 2S, 29, which may be arranged opposing as shown, that the resultant etl'ect ot' coils 26, 2T is dependent on IV-Igr which equals Il and similarly the resultant eiiect ot coils 28, 29 is proportional to Iza-I1, which equals I3. My invent-ion is, ot' course, not limited to this arrangement but obviously includes the use of current transt'mmers or auto-transformers having equal or unequal transformation ratios for the two currents I and I', and the sum or di'erence of the secondary currents may be ted to the winding ot each electro-magnet and also the use ot transformers with two primaries having equal or unequal coil turns :ted by the currents I and I may likewise be utilized.

I claim:

l. In an electroresponsive device for an electric circuit, a movable member and means for controlling the movement thereof in accordance with a resultant oi a plurality of dili'erent predetermined functions of at least two of the phase sequence components of the power of said circuit.

Q. In an eleetroresponsive device for an electric circuit, a. movable member and means 'rer controlling the movement thereof in accordance with the difference between two different predetermined Jfunctions of a plurality ot' the phase sequence components of the power et said circuit.

3. In an electroresponsive device for an electric circuit, a movable member, means for exertingr thereon an effect dependent on the sum oit at least two of the phase sequence components of the power of the circuit and means for exerting on said member an opposing eect dependent on the difference between the positive and negative phase sequence components ol the power' ot the circuit.

4. In a elect-roresponsive device for an electric circuit, a movable member, means for controlling said member in accordance with the total power ot the circuit and opposing means for controlling said member in accordance with the difference between the positive and negative phase sequence components of the power of the circuit.

5. In an electroresponsive device for an (-lectric circuit, a rotatable member, and means tor exerting thereon a torque substantially proportional to (Pd-lP-l- PO) and an opposing torque substantially proportional to (1)*10 where Pd, Pi, and P0 are respectively the positive, negative and zero phase sequence components of the power ot` the circuit.

6. In combination, means for exerting an effect dependent on a predetermined function of a plurality of the phase sequence components of the power of an electric circuit, cooperating means for exerting an effect dependent on a different predetermined function ol a plurality ofthe phase sequence components of the power of the circuit and means controlled by the conjoint action of said exerting means.

7. In combination, means for exerting an effect dependent on a function of the sum of at least two of the phase sequence components of the power of an electric circuit, cooperating means or exerting an opposing effect dependent on a function of the dill'erence between the positive and negative phase sequence components of the power ol the circuit and means controlled by the conjoint action of said exerting means in accordance with the ditference between the effects exerted thereby.

8. An electroresponsive device including rotatably mounted induction disk means and electromagnetic means for exerting thereon a` torque dependent ou the ditl'erence between two .flili'erent predetermined functions ol a plurality of the phase sequence components of the power of an electric circuit.

9. In combination, means for exerting an eil'ect dependent on the function of the sum ot at least two el the phase sequence components of the power of an electric circuit, cooperating means for exerting an effect dependent on a function of the difference between two of the phase sequence components of the power of the circuit and means controlled bythe conjoint action of said exerting means in accordance with a resultant of the etl'ects exerted thereby.

IUS

lll)

10. In combination, a movable member and means for actuating the member in accordance with at least one of the phase sequence components of the power' of an electric circuit, including electro-magnetic means for controlling said member in accordance with the total power of the circuit and cooperating electro-magnetic means for controlling said member in accordance with the difference between the positive and negative phase sequence components of the power of the circuit.

l1. In combination, a movable member and means for actuatingr said member in aoco-rdance with the sum of the negative and zero phase sequence components of the power of an electric circuit including means for controlling said member in accordance with the sum of the positive, negative and zero phase sequence components of the circuit and cooperating` Aopposing means for controlling the member in accordance with the difference between the positive and negative phase sequence components of the power of the circuit.

12. An electroresponsive device including rotatably mounted induction disk means and electro-n'iagnetic means inductively associated with said disk means and arranged to exert thereon a torque proportional to the difference between two different predetermined functions of a plurality of the phase sequence components of the power of yan electric circuit.

18. In combination with an electric circuit, an electroresponsive device including rotatably mounted induction disk means, electro-magnetic means inductively associated with said disk means and connected and arranged to exert thereon a torque proportional to the sum of at least two of the phase sequence components of the power of the circuit and cooperating electro-magnetic means inductively associated with said disk means and connected and arranged to exert thereon an opposing torque proportional 'to the difference between two of the phase sequence components of the power of the circuit.

14. In combination with an electric circuit, an electroresponsive device including rotatabl mounted induction disk means and means or controlling the rotation of said disk means in accordance with at least one of the phase sequence components of the power of the circuit including electro-magnetic motor means inductively associated with the disk means and connected and arranged to exert thereon a torque proportional to the total power of the circuit and cooperating electro-magnetic means inductively associated with said disk means and connected and arranged to exert thereon an opposing torque proportional to the difference between the positive and negative phase sequence components of the power of the circuit.

15. In an electroresponsive device for a three-phase electric circuit, rotatably mounted member, means for exerting thereon three torques respectively proportional to the products ofthe currents in the three circuit conductors, the voltages to ground of the respective conductors and the cosines of the phase angles between the respective currents and voltages, and opposing means for exerting on said member three torques respectively proportional to the products of the currents in the three circuit conductors, the line to line voltages in quadrature to said currents under balanced circuit conditions and the sines of the phase angles between the respective currents and voltages.

16. The method of utilizing the phase sequence components of the power of a polyphase circuit which includes producing two forces respectively dependent on two different predetermined functions of a plurality of the phase sequence components of the power of the circuit and combining said forces to diminish the eect of one of said phase sequence components.

` 17. The method of utilizing the phase sequence components of the power of a polyphase circuit which inclu-des producing two forces respectively dependent on 'two different predetermined functions of a plurality of the phase sequence components of the power of the circuit and combining said forces to diminish 'the effect of one of said phase sequence components relatively to another by a definite ratio.

18. The method of utilizing the phase sequence components of the power of a polyphase circuit which includes producing two forces respectively dependent on a function of the sum of the phase sequence components of the power of the circuit and a function of the difference between two of the phase sequence compone-nts of the power of the circuit and combining said forces to diminish the effect of one of said phase sequence components relatively to another by a definite ratio.

19. The method of utilizing the phase sequence components of the power of a polyphase circuit which includes producing two forces respectively equal. to 7c1 (Pd-PF1 Pn) and 7a2 (Pd-Pi) where 701 and 7a2 are constants and Pd, Pi and Po are respectively the positive, negative and zero phase sequence coniponents of the power of the circuit and combining said forces to diminish the effect of one of said phase sequence components in accordance with the relative values of 7:l and 762.

20. In combination, a movable member,

means for exerting thereon a force dependent' said member arranged to reduce the effect of one of said phase sequence. Components, said cooperating means being arranged to exert on said member a force dependent on a dl'fercnt predetermined function 0f a plurality of the phase sequence components of the power of the circuit.

AVR-AM DAVID ILIOVICI.

Certicate 0f Correction Patent No. 1,816,778. y GrantedJuly 28, 1931, to

AVRAM DAVID ILIOVICI. It is hereby certified that error appears in the printed specification of the above numbered patent requiring correction as follows z Page 2, lines 106 to 109, should read p (9) P' (Esa-EQ I1al Sin 19,1., (E1" Esd) I2d Sill l5/2d l (E2d E1d I3d sin (blgd-l (Eg E2) 11i Sin qblli instead of as shown; and that the said Letters Patent should be read with this correction therein that the same may conform to the record of the case in the Patent Ofice.

Signed and sealed this 15th day of September, A. D. 1931.

[SEAL] M. J. MOORE,

Act/ng ommz'ssz'oner of Patents.

Certificate of Correction Patent No. 1,816,778. l Granted July 28, 1931, to

' AVRAM DAVID ILIOVICI.

It is hereby certified that error appears in the printed speciication of the above numbered patent requiring correction as follows Page 2, lines 106 to 109,:sh0u1d read (9) P (Esa-E29 I1rl Sin ld +(E1-E3)I2d Sin l2d i (Ezd E111) I3d Sin 3d i (Egi- E25) I1 Sin @alli instead of as shown; and that the said Letters Patent should be read with this correction therein that the same may conform to the record o the case in the Patent OHice.

Signed and sealed this 15th day of September, A. D. 1931.

[SEAL] M. J. MOORE,

Acting 00m/mission@1 of Patents. 

